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author | schnetter <schnetter@578cdeb0-5ea1-4b81-8215-5a3b8777ee0b> | 2005-12-11 05:42:55 +0000 |
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committer | schnetter <schnetter@578cdeb0-5ea1-4b81-8215-5a3b8777ee0b> | 2005-12-11 05:42:55 +0000 |
commit | 45896374e265416036c14fdb596de6dc8f9f07ef (patch) | |
tree | 2de39d84665f327eda59b9aed0707fc7162b6582 | |
parent | 80eb9c1a93995961c98189fa4c62fe9558bf8777 (diff) |
Correct unimportant typographical error
git-svn-id: http://svn.cactuscode.org/arrangements/CactusNumerical/MoL/trunk@98 578cdeb0-5ea1-4b81-8215-5a3b8777ee0b
-rw-r--r-- | doc/documentation.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/doc/documentation.tex b/doc/documentation.tex index 35c85ed..29841d8 100644 --- a/doc/documentation.tex +++ b/doc/documentation.tex @@ -657,7 +657,7 @@ intermediate steps before averaging: \end{eqnarray} The Runge-Kutta methods are those typically used in hydrodynamics by, -e.g., Shu and others - see~\cite{CactusBase_MoL_Shu99} for +e.g., Shu and others --- see~\cite{CactusBase_MoL_Shu99} for example. Explicitly the first order method is the Euler method: \begin{eqnarray} \label{CactusBase_MoL_eq:rk1} |